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The Quantum Mechanical Atom CHAPTER 8 Chemistry: The Molecular Nature of Matter, 6 th edition By Jesperson, Brady, & Hyslop
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CHAPTER 8: Quantum Mechanical Atom 2 Learning Objectives Light as Waves, Wavelength and Frequency The Photoelectric Effect, Light as Particles and the Relationship between Energy and Frequency Atomic Emission and Energy Levels The Bohr Model and its Failures Electron Diffraction and Electrons as Waves Quantum Numbers, Shells, Subshells, and Orbitals Electron Configuration, Noble Gas Configuration and Orbital Diagrams Aufbau Principle, Hund’s Rule, and Pauli Exclusion Principle, Heisenberg Uncertainty Principle Valence vs Inner Core Electrons Nuclear Charge vs Electron Repulsion Periodic Trends: Atomic Radius, Ionization Energy, and Electron Affinity
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Particle-Wave Duality Light Exhibits Interference Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 3 Constructive interference –Waves “in-phase” lead to greater amplitude –They add together Destructive interference –Waves “out-of-phase” lead to lower amplitude –They cancel out
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Particle-Wave Duality Are Electrons Waves or Particles? Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 4 Light behaves like both a particle and a wave: –Exhibits interference –Has particle-like nature When studying behavior of electrons: –Known to be particles –Also demonstrate interference
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Particle-Wave Duality Standing vs Traveling Waves Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 5 Traveling wave –Produced by wind on surfaces of lakes and oceans Standing wave –Produced when guitar string is plucked –Center of string vibrates –Ends remain fixed
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Particle-Wave Duality Standing Wave on a Wire Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 6 Integer number (n) of peaks and troughs is required Wavelength is quantized: L is the length of the string
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Particle-Wave Duality Standing Wave on a Wire Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 7 Has both wave-like and particle-like properties Energy of moving electron on a wire is E =½ mv 2 Wavelength is related to the quantum number, n, and the wire length:
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Particle-Wave Duality Electron on a Wire Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 8 Standing wave Half-wavelength must occur integer number of times along wire’s length de Broglie’s equation relates the mass and speed of the particle to its wavelength m = mass of particle v = velocity of particle
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Particle-Wave Duality Electron on a Wire Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 9 Starting with the equation of the standing wave and the de Broglie equation Combining with E = ½mv 2, substituting for v and then λ, we get Combining gives:
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Particle-Wave Duality De Broglie & Quantized Energy Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 10 Electron energy quantized – Depends on integer n Energy level spacing changes when positive charge in nucleus changes – Line spectra different for each element Lowest energy allowed is for n =1 Energy cannot be zero, hence atom cannot collapse
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Particle-Wave Duality Ex: Wavelength of an Electron Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 11 What is the de Broglie wavelength associated with an electron of mass 9.11 × 10 –31 kg traveling at a velocity of 1.0 × 10 7 m/s? = 7.27 × 10 –11 m
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Particle-Wave Duality Ex: Wavelength of an Electron Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 12 Calculate the de Broglie wavelength of a baseball with a mass of 0.10 kg and traveling at a velocity of 35 m/s. A. 1.9 × 10 –35 m B. 6.6 × 10 –33 m C. 1.9 × 10 –34 m D. 2.3 × 10 –33 m E. 2.3 × 10 –31 m
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Particle-Wave Duality Wave Functions Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 13 Schrödinger’s equation – Solutions give wave functions and energy levels of electrons Wave function – Wave that corresponds to electron – Called orbitals for electrons in atoms Amplitude of wave function squared – Can be related to probability of finding electron at that given point Nodes – Regions where electrons will not be found
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Quantum Numbers Orbitals Characterized by 3 Quantum #’s Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 14 Quantum Numbers: – Shorthand – Describes characteristics of electron’s position – Predicts its behavior n = principal quantum number – All orbitals with same n are in same shell ℓ = secondary quantum number – Divides shells into smaller groups called subshells m ℓ = magnetic quantum number – Divides subshells into individual orbitals
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Quantum Numbers Principal Quantum Number (n) Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 15 Allowed values: positive integers from 1 to – n = 1, 2, 3, 4, 5, … Determines: – Size of orbital – Total energy of orbital R H hc = 2.18 × 10 –18 J/atom For given atom, – Lower n = Lower (more negative) E = More stable
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Quantum Numbers Orbital Angular Momentum ( ℓ ) Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 16 – Allowed values: 0, 1, 2, 3, 4, 5…(n – 1) – Letters: s, p, d, f, g, h Orbital designation number nℓ letter Possible values of ℓ depend on n – n different values of ℓ for given n Determines Shape of orbital
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Quantum Numbers Magnetic Quantum Number (m ℓ ) Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 17 Allowed values: from –ℓ to 0 to +ℓ – Ex. when ℓ=2 then m ℓ can be –2, –1, 0, +1, +2 Possible values of m ℓ depend on ℓ – There are 2ℓ+1 different values of m ℓ for given ℓ Determines orientation of orbital in space To designate specific orbital, you need three quantum numbers – n, ℓ, m ℓ
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Quantum Numbers n, ℓ, and m ℓ Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 18
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Quantum Numbers Multiple Electrons in Orbitals Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 19 Orbital Designation Based on first two quantum numbers Number for n and letter for ℓ How many electrons can go in each orbital? Two electrons Need another quantum number
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Quantum Numbers Spin Quantum Number (m s ) Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 20 Arises out of behavior of electron in magnetic field electron acts like a top Spinning charge is like a magnet – Electron behave like tiny magnets Leads to two possible directions of electron spin – Up and down – North and south Possible Values: +½ ½
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Quantum Numbers Pauli Exclusion Principle Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 21 No two electrons in same atom can have same set of all four quantum numbers (n, ℓ, m ℓ, m s ) Can only have two electrons per orbital Two electrons in same orbital must have opposite spin – Electrons are said to be paired
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Quantum Numbers Number of Orbitals Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 22
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Quantum Numbers Magnetic Properties Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 23 Two electrons in same orbital have different spins – Spins paired—diamagnetic – Sample not attracted to magnetic field – Magnetic effects tend to cancel each other Two electrons in different orbital with same spin – Spins unpaired—paramagnetic – Sample attracted to a magnetic field – Magnetic effects add Measure extent of attraction – Gives number of unpaired spins
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Quantum Numbers Ex: Number of Electrons Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 24 What is the maximum number of electrons allowed in a set of 4p orbitals? A. 14 B. 6 C. 0 D. 2 E. 10
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Electron Configurations Ground State Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 25 1s1s2s2s2p2p Electron Configurations Distribution of electrons among orbitals of atom 1.List subshells that contain electrons 2.Indicate their electron population with superscript e.g. N is 1s 2 2s 2 2p 3 Orbital Diagrams Way to represent electrons in orbitals 1.Represent each orbital with circle (or line) 2.Use arrows to indicate spin of each electron e.g. N is
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Electron Configurations Energy Level Diagram Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 26 How to put electrons into a diagram? Need some rules
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Electron Configurations Aufbau Principle Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 27 Building-up principle Pauli Exclusion Principle Two electrons per orbital Fill following the order suggested by the periodic table Spins must be paired
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Electron Configurations Hund’s Rule Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 28 If you have more than one orbital all at the same energy – Put one electron into each orbital with spins parallel (all up) until all are half filled – After orbitals are half full, pair up electrons Why? Repulsion of electrons in same region of space Empirical observation based on magnetic properties
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Electron Configurations Orbital Diagram & Electron Configurations: e.g. N, Z = 7 Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 29 Each arrow represents electron 1s 2 2s 2 2p 31s 2 2s 2 2p 3
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Electron Configurations Orbital Diagram and Electron Configurations: e.g. V, Z = 23 Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 30 Each arrow represents an electron 1s 2 2s 2 2p 2 3s 2 3p 2 4s 2 3d 31s 2 2s 2 2p 2 3s 2 3p 2 4s 2 3d 3
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Electron Configurations Ex: Orbital Diagrams & Electron Configurations Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 31 Give electron configurations and orbital diagrams for Na and As Na Z = 11 As Z = 33 1s 2 2s 2 2p 2 3s 11s 2 2s 2 2p 2 3s 1 1s 2 2s 2 2p 6 3s 2 3p 6 4s 2 3d 10 4p 3
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Electron Configurations Ex: Ground State Electron Configurations Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 32 What is the correct ground state electron configuration for Si? A. 1s 2 2s 2 2p 6 3s 2 3p 6 B. 1s 2 2s 2 2p 6 3s 2 3p 4 C. 1s 2 2s 2 2p 6 2d 4 D. 1s 2 2s 2 2p 6 3s 2 3p 2 E. 1s 2 2s 2 2p 6 3s 1 3p 3
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Problem Set B
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